(a) Take the D-T nuclear reaction : `""_(1)^(2)H+""_(1)^(3)H rarr ""_(2)^(4)He+n`
It is given that:
Mass of `""_(1)^(2)H,m_(1)=2.014102 u`
Mass of `""_(1)^(3)H,m_(2)= 3.016049 u `
Mass of `""_(2)^(4)H,m_(3)=4.002603u`
Mass of `""_(0)^(1)n,m_(4)=1.008665 u`
Q-value of the given-T reaction is :
`Q=[m_(1)+m_(2)-m_(3)-m_(4)]c^(2)`
`=[2.014102+3.016049-4.002603-1.008665]c^(2)`
`=[0.018883 c^(2)]u`
But 1 u=931.5 MeV/`c^(2)`
`therefore Q=0.018883xx931.5=17.59 MeV`
(b) Radius of deuterium and tritium , `r~~2.0 " " fm=2xx10^(-15)m`
Distance between the two nuclei at the moment when they touch each other,d `=r+r=4xx10^(-15)m`
Charge on the deuterium nucleus=e
Charge on the tritium nucleus=e
Hence, the repulsive potential energy between the two nuclei is given as :
`V=(e^(2))/(4pt in_(0)(d))`
Where, `in_(0)`= Permittivity of free space
`(1)/(4 pi in_(0))=9xx10^(9)Nm^(2)C^(-2)`
`therefore V=(9xx10^(9)xx(1.6xx10^(-19))^(2))/(4xx10^(-15))=5.76xx10^(-14)J`
`(5.76xx10^(-14))/(1.6xx10^(-19))=3.6xx10^(5) eV=360keV`
Hence, `5.76xx10^(-14)J` or 360keV of kinetic energy (KE) is needed to overcome the Coloumb repulsion between the two nuclei.
However, it is given that:
`KE=2xx(3)/(2)kT`
Where, k=Boltzmann constant`=1.38xx10^(-23) m^(2)kg s^(-2)K^(-1)`
T= Temperature rquired for triggering the reaction
`thereforeT=(KE)/(3K)`
`=(5.76xx10^(-14))/(3xx1.38xx10^(-23))=1.39xx10^(9) K`
Hence, the gas must be heated to a temperature of `1.39xx10^(9)`K t initiate the reaction.